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Title: Possible excitonic phase of (Pr1-yRy)1-xCaxCoO3 (R = Lanthanides and Y)

Abstract

(Pr1-yRy)1-xCaxCoO3 (R = Y and/or Lanthanide elements) exhibits a “hidden order transition” in the (x, y) region near (0.5, 0.0) at temperature Ts, where none of magnetic ordering and change of the space group have been found, even though significant anomalies in various physical quantities exist. When the (x, y) is outside of the above region, the transition can essentially be understood by the spin-state-crossover of isolated Co atoms. To study whether excitonic condensation (EC) recently proposed is relevant to the “hidden order transition”, we measured magnetic excitation spectra χ” (Q, ω) by means of inelastic neutron scattering on a single crystal of (Pr0.8Y0.2)0.7Ca0.3CoO3, and obtained following results: While the spectra from the Co 3d electrons observed at 200 K (>above Ts) have characteristics of ordinary strongly correlated electron systems, the χ” (Q, ω) - ω curve at 4 K (<Ts) has a feature reminiscent, at first sight, of a weak pseudogap-like structure. This result can be explained by the realization of the EC phase or “EIQ” phase or at least by the picture that the system is in the boundary region between the low-spin and EQI"phases. Finally, this result strongly suggests that there exists the EIQ phase in themore » present sample or at least in (Pr1–yRy)1–xCaxCoO3 with (x, y) near (0.5, 0.0).« less

Authors:
 [1];  [1]; ORCiD logo [2];  [3]
  1. Comprehensive Research Organization 
for Science and Society (CROSS), Ibaraki (Japan)
  2. Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States)
  3. Nagoya Univ., Nagoya (Japan)
Publication Date:
Research Org.:
Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States)
Sponsoring Org.:
USDOE Office of Science (SC), Basic Energy Sciences (BES)
OSTI Identifier:
1489095
Grant/Contract Number:  
AC05-00OR22725
Resource Type:
Accepted Manuscript
Journal Name:
Physica. B, Condensed Matter
Additional Journal Information:
Journal Volume: 551; Journal Issue: C; Journal ID: ISSN 0921-4526
Publisher:
Elsevier
Country of Publication:
United States
Language:
English
Subject:
75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY; Excitonic condensation; Perovskite cobalt oxides; Hidden order; Magnetic excitation spectra; Neutron scattering

Citation Formats

Moyoshi, Taketo, Kamazawa, Kazuya, Matsuda, Masaaki, and Sato, Masatoshi. Possible excitonic phase of (Pr1-yRy)1-xCaxCoO3 (R = Lanthanides and Y). United States: N. p., 2017. Web. doi:10.1016/j.physb.2017.11.055.
Moyoshi, Taketo, Kamazawa, Kazuya, Matsuda, Masaaki, & Sato, Masatoshi. Possible excitonic phase of (Pr1-yRy)1-xCaxCoO3 (R = Lanthanides and Y). United States. https://doi.org/10.1016/j.physb.2017.11.055
Moyoshi, Taketo, Kamazawa, Kazuya, Matsuda, Masaaki, and Sato, Masatoshi. Thu . "Possible excitonic phase of (Pr1-yRy)1-xCaxCoO3 (R = Lanthanides and Y)". United States. https://doi.org/10.1016/j.physb.2017.11.055. https://www.osti.gov/servlets/purl/1489095.
@article{osti_1489095,
title = {Possible excitonic phase of (Pr1-yRy)1-xCaxCoO3 (R = Lanthanides and Y)},
author = {Moyoshi, Taketo and Kamazawa, Kazuya and Matsuda, Masaaki and Sato, Masatoshi},
abstractNote = {(Pr1-yRy)1-xCaxCoO3 (R = Y and/or Lanthanide elements) exhibits a “hidden order transition” in the (x, y) region near (0.5, 0.0) at temperature Ts, where none of magnetic ordering and change of the space group have been found, even though significant anomalies in various physical quantities exist. When the (x, y) is outside of the above region, the transition can essentially be understood by the spin-state-crossover of isolated Co atoms. To study whether excitonic condensation (EC) recently proposed is relevant to the “hidden order transition”, we measured magnetic excitation spectra χ” (Q, ω) by means of inelastic neutron scattering on a single crystal of (Pr0.8Y0.2)0.7Ca0.3CoO3, and obtained following results: While the spectra from the Co 3d electrons observed at 200 K (>above Ts) have characteristics of ordinary strongly correlated electron systems, the χ” (Q, ω) - ω curve at 4 K (<Ts) has a feature reminiscent, at first sight, of a weak pseudogap-like structure. This result can be explained by the realization of the EC phase or “EIQ” phase or at least by the picture that the system is in the boundary region between the low-spin and EQI"phases. Finally, this result strongly suggests that there exists the EIQ phase in the present sample or at least in (Pr1–yRy)1–xCaxCoO3 with (x, y) near (0.5, 0.0).},
doi = {10.1016/j.physb.2017.11.055},
journal = {Physica. B, Condensed Matter},
number = C,
volume = 551,
place = {United States},
year = {Thu Nov 23 00:00:00 EST 2017},
month = {Thu Nov 23 00:00:00 EST 2017}
}

Journal Article:
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Figures / Tables:

Fig. 2 Fig. 2: Examples of the data analysis. At 200 K, the Lorentzian spectral shape ħΓQω/[ħ2ω 2+ΓQ2] (thick dashed line) is fitted to the observed data (open squares). At 4 K, the sum of the spectra from Co electrons with the shape ħΓQω/[ħ2(ω - ωQ)2 + ΓQ2] (thick solid line) andmore » those from the crystal field excitation of Pr ions (thin solid Gaussian line) is fitted to the observed data (closed circles). Note that above ~10 meV, the black dots coincide with the thick solid line.« less

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